JP5383651B2 - Apparatus for quench protection and damping stabilization in quasi-permanent superconducting magnets. - Google Patents

Abstract

A superconducting magnet assembly comprises a superconducting magnet which, under working conditions, generates a magnetic field in a working volume. The superconducting magnet is connected in parallel with a series combination of a superconducting fault current limiter and a resistor, and with a DC power source. Under working conditions, the magnet can be energized by the power source to generate a desired magnetic field in the working volume.

Description

  The present invention relates to stabilizing damping of superconducting magnets operating in quasi-permanent mode, and quench protection of such magnets.

  A typical superconducting magnet system consists of a main magnet coil that produces the desired magnetic field strength, and a superconducting switch that is mounted in parallel with the coil to allow a permanent mode of operation.

  The superconducting magnet normally operates in a permanent mode, during which current is introduced from the power source into the superconducting coil via a current lead using a ramp-up procedure while the switch is open. The superconducting switch is then closed and current continues to flow through the superconducting coil for a relatively long time. As a result, a stationary magnetic field is generated. However, it is not necessary to continuously supply power to the magnet by the current source. By closing the superconducting switch, thus allowing the current to circulate in the continuous superconducting loop formed by the magnet and the switch, and by dampening the lead current to zero, the magnet is in a permanent mode.

  After the current lead current decays to zero, the current lead is generally completely removed. As a result, current can circulate continuously through the superconducting loop formed by the magnets and switches. As is known in such conventional permanent mode magnets, the current drifts with time and the magnet is characterized by a damping performance that is highly dependent on the resistance of the superconducting joint. As for the attenuating magnet, a stabilization solution using a resistance circuit in conjunction with a superconducting switch as described in US 2003/0057942 has been developed and successfully realized in a superconducting magnet. The resistor stabilization solution in conjunction with the switch described in the above patent application is in particular a protection circuit comprising an array of resistors and / or diodes generally connected to the terminals of each section of at least some sections of the magnet Applies to magnets that are protected in multiple sections. A conventional superconducting switch provided as part of a superconducting magnet circuit is similarly protected. These types of magnets are typically energized by a power source that is typically rated in the hundreds of amps and has a relatively low compliance voltage, typically on the order of 10V.

  As shown in FIG. 1, a superconducting magnet 1 generally carries superconducting switches 3 in parallel. During energization, a heater (not shown) incorporated in the switch is used so that the magnet 1 can be energized up to the set current by increasing the magnitude of the current applied from the power source 4. The switch 3 enters the resistance mode. The relatively large resistance of the switch 3 in the resistance mode limits the current passing through the switch and virtually all current flows straight through the magnet 1. Once the required magnet operating current is reached, the switch heater is turned off and the superconducting switch 3 returns to the superconducting state. The current in the current lead is reduced until it reaches zero. The current flowing in the magnet 1 circulates in the superconducting loop formed by the switch 3 and the magnet 1. Once the current in the current lead has dropped to zero, the power supply 4 can now be switched off and completely removed.

  As is well known in the art, superconducting magnets are susceptible to quench events. When such an event occurs, for some reason, part of the magnet is no longer superconducting. For example, this may occur due to local heating caused by events related to the movement of a single short wire or the structural integrity of the coil. The part that is no longer superconducting becomes resistance. The current flowing through the magnet causes heating of this resistive portion, which in turn heats more superconducting wire, turns that more superconducting wire into resistance, and thus heat propagates to the rest of the magnet. The effect of this is that the energy stored in the magnet is dissipated as the heat of the wire of the magnet coil. In addition, the resulting drop in current flowing through the magnet inductance creates a high voltage at the magnet terminals. During the quench, the current, voltage, and temperature all increase. These are so high that it is known that poorly protected magnets (and switches) are prone to damage. Therefore, a protection circuit is generally provided to prevent and manage quenching.

  Known superconducting magnets, such as MRI, NMR imaging, particle accelerators, and superconducting magnets intended for research physics are generally constructed by several coils and sections within the coils. Two major strategies for quench protection are commonly employed. First, it is expected that a single protection circuit will provide protection for the entire magnet. Such circuits are typically provided with a single protective resistor or resistor network, either inside or outside the cryostat that houses the superconducting magnet. Alternatively, a protection circuitry is constructed using a network of resistors and / or diodes to protect individual coils or coil sections within the magnet and / or switch. This second configuration is intended for improvement by US Patent Application Publication No. 2003/0057942. The use of an individual protection resistor usually means that the protection resistor is in the cryostat, but the protection resistor can also be placed outside the cryostat, while using a single resistor The configuration generally places the resistor outside of the cryostat, but correspondingly, a single resistor could be placed in the cryostat. Such an external protective resistor adds the problem of passing the conductor out of the cryostat, but the heat dissipated by the resistor during the quench does not consume the cryogen or heat is contained in the cryostat. Has the advantage of not introducing.

  During the quench, the superconducting switch is brought into a normal or resistive state by a process familiar to those skilled in the art, and the remaining current is sent to the protection circuit of the switch, thereby dissipating the energy stored in the magnetic field.

  If the entire magnet is protected with a single resistor connected to its terminals, considering that the superconducting magnet operates with a permanent current of several hundred amperes, the result is probably very high, on the order of a few kilovolts Voltage can also be generated across the combination of switch 3 and resistor 5 used between the terminals of the magnet and thus in the stabilization circuit. Superconducting switches are generally not designed to withstand such high voltages and are therefore destroyed. In order to prevent destruction of the superconducting element, a protection circuit mechanism is generally provided as a part of the superconducting switch. Such protection circuitry may take the form of a diode and / or resistor parallel circuit to the switch itself. Nevertheless, superconducting switches can only withstand voltages of tens of volts.

  The superconducting switch 3 is generally limited in how much current it can carry (usually several hundred amperes) and how much voltage it can tolerate (typically only a few tens of volts). The superconducting switch 3 is usually protected by a diode and / or a resistor. Since the protection of the switch is typically a ratio of, for example, tens to hundreds to one, most of the current flows through the quench protection circuit when the switch is in a resistive state during the quench. As a result, the current flowing through the switch during the quench is very small, and therefore the heat dissipated through it is kept to a minimum. If the switch is not properly protected, it will burn out and the magnet and / or switch will have to be repaired or replaced.

  With reference to FIGS. 1 and 2, US 2003/0057942 describes a method and arrangement for stabilizing magnetic field attenuation in a superconducting magnet. Previously, a superconducting magnet was energized during ramp-up and then shorted by a superconducting switch when the current through the magnet reached the desired value. In US 2003/0057942, a resistor 5 is added in series with the superconducting switch 3 and the current rises slightly above the normal operating current as shown in the procedure of FIG. This allows the algebraic sum of the voltage of the circuit defined by the magnets, switches and resistors to be adjusted to be near or near zero, the condition required for zero field drift. Although protective resistors are not shown in FIGS. 1 and 2, this solution is particularly applicable to magnets having separate protection circuits for the various sections of the magnet.

  In particular, US Patent Application Publication No. 2003/0057942 includes a superconducting magnet 1 that generates an operating magnetic field under operating conditions, the superconducting magnet being connected in parallel with the superconducting switch 3, and the switch and the magnet being a power source. 4 is adapted to be connected in parallel so that the magnet can be energized by the power supply to generate the desired amount of magnetic field with the switch 3 open under operating conditions (ie resistance mode). The switch 3 is then closed (i.e. returned to the superconducting mode), describing the superconducting magnet assembly. In particular, the assembly further comprises a resistor 5 connected in series with the switch 3, which is connected together in parallel to each of the magnet 1 and the power supply 4. Resistor 5 may have a resistance in the range of 1 to 1000 times, preferably 10 to 100 times that of the magnet schematically represented as resistance 2 in FIG. The power source 4, the magnet 1, and the resistor 2 can be configured such that the instability of the magnetic field generated during use is less than 10 ppm / hour, more preferably less than 0.01 ppm / hour.

US 2003/0057942 is also a method of energizing such a superconducting magnet assembly, comprising:
i) opening the switch 3 and energizing the magnet 1 from the power source 4;
ii) closing switch 3;
iii) changing the current supply from the power source 4 so as to reduce the drift of the magnetic field generated by the operation amount;
Also described is a method comprising:

  The method can further include the steps iv) of monitoring the magnetic field attenuation, and repeating steps iii) -iv) with different current changes in step iii) to reduce the magnetic field attenuation.

  To provide a more complete background of the present invention, the teachings of US Patent Application Publication No. 2003/0057942 are primarily reproduced below.

  There are many applications where superconducting magnets are used to generate a magnetic field with a stable amount of operation. Examples include MRI, NMR, ICR, and cyclotron, where the magnet operates in a so-called “permanent mode”. This includes that once the magnet is energized, a connection close to zero ohms is connected between the beginning and end of the magnet. Techniques for accomplishing this are well known. The resulting magnetic field stability is then determined by the time constant of the magnet inductance and total circuit resistance.

  The time constant is defined as L / R. Where L is the magnet inductance in Henry units, R is the total circuit resistance in ohms, and the time constant is measured in seconds.

  Thus, unless L = ∞ or R = 0Ω, the resulting time constant is finite, resulting in exponential decay of both magnet current and magnetic field over time.

  In some applications, it is desirable to have an attenuation factor as close to zero as possible. In general, it is preferable for the NMR application to have an attenuation rate of less than 0.01 ppm / hour.

  In many systems, the magnet inductance is fixed by the shape required to produce the very high degree of uniform magnetic field and operating current required. Therefore, in practice, the circuit resistance of the magnet determines the magnetic field attenuation rate.

  This magnetic drift has been a recognized problem for some time and the only solution has been to re-energize the magnet.

  The problems described above with respect to magnetic field drift are overcome by adding a resistor in series with the switch. This allows the algebraic sum of the voltage of the circuit defined by the magnets, switches and resistors to be adjusted to be near or near zero, the condition required for zero field drift.

  Once the switch is closed, the power supply must remain connected, in contrast to conventional systems where the power supplied to the magnet circuit is reduced to zero, but achieves a stable magnetic field for a very long period of time. This advantage is thought to outweigh the cost of maintaining the power supply.

  Generally, the resistor has a resistance that is at least 10 to 100 times greater than the resistance of the magnet, although resistances in the range of 1 to 1000 times the magnet resistance are possible. In addition, the resistor must have substantially zero inductance.

  There are various ways in which the correct current can be determined to achieve zero magnetic field drift.

In the first method, the resistance of the magnet can be determined. This is done by providing a second superconducting switch in parallel with the magnet and the power supply so that once the magnet is powered up to the required field strength, the second switch is closed and then the field attenuation is monitored to determine the value of the magnet resistance. By obtaining, it can be easily achieved. Attenuation rate = 1 / time constant, and the time constant is also L / R (where L is a magnet inductance, and R is a magnet resistance). Therefore, magnet resistance R = damping rate (ppm / second) × magnet inductance L. For example, when L = 100H and attenuation factor = 3.6 ppm / hour, that is, 3.6 × 10 ⁻⁶ / 3600 = 10 ⁻⁹ seconds, inductance L = 100H and R = 10 ⁻⁷ ohm.

  In the second method, a voltmeter can be attached to the magnet and the resistance can be determined directly in response to the passage of a known current.

In the third approach, the method further includes:
iv) monitoring magnetic field attenuation, and repeating steps iii) -iv) with different current changes in step iii) to reduce magnetic field attenuation;
including. This iterative technique avoids the need for additional components.

  The magnet can have any conventional structure utilizing one or both of low and high temperature superconducting materials or other materials with low bulk resistance. Since the power supply remains connected to the magnet, a high temperature superconducting current lead is preferred to reduce heat conduction and minimize heat release in the environment.

As shown in FIG. 1, the assembly comprises a conventional form of superconducting magnet 1, the resistance R ₁ of the magnet being shown separately at 2. The magnet is connected in parallel with the superconducting switch 3 and the power source 4. The components described so far are conventional. In such a conventional system, the switch 3 is initially open and the magnet 1 is powered up by the power source 4 until it generates an operational amount of the required magnetic field. The superconducting switch 3 is then closed, but current does not begin to flow through the switch 3 until the power source 4 gradually stops operating. Due to this deactivation, current flows in a “permanent mode” through the series circuit formed by the magnet 1 (including the resistor R ₁ ) and the switch 3. However, as explained above, due to the specific resistance 2 (R ₁ ) of the magnet 1, the operating magnetic field generated by the magnet 1 gradually drifts or attenuates.

  This is overcome in the present invention by inserting an additional resistor 5 (R2) in series with the superconducting switch 3.

Referring now to FIG. 2, with switch 3 open, magnet 1 is energized to normal operating current I (step 10), then switch 3 is closed (step 11), and then a resistor in series with switch 3 is connected. Until the additional current flowing in the device 5 is equivalent and has a reverse polarity voltage, and the resistance voltage generated in the magnet 1 is strictly canceled, that is, until the algebraic sum of the circuit voltage becomes zero, the current is ΔI Further increased (step 12)
It should be understood that the increased power supply current does not flow to magnet 1 (switch 3 is closed), but only to switch 3 and resistor 5. This is because once the switch 3 is closed, the change in the current of the power source is divided and flows into both the switch circuit and the magnet circuit. The ratio between the two currents is determined by the inverse ratio of the circuit inductance. Since the magnet has a very large inductance (typically 100H) and the switch inductance is very small (typically 100 nanohenries), the current ratio is ^10-9 , so all practical considerations are All power supply current changes flow to the switch circuit. It should also be noted here that, unlike in the permanent mode, during operation of the magnet 1, the power supply unit 4 remains connected and supplies the current I + ΔI to the circuit.

The desired state for magnetic field stability is when the magnet voltage drops and the magnet-switch loop resistor 5 is equivalent and reverse, ie I · R (magnet) = ΔI · R (resistor 5). 1]
This is the case.

  Small variations in power supply are filtered by the time constants of circuit resistance and magnet inductance, so the time rate of change of the resulting magnetic field is determined by the time constant of the magnet operating in “permanent mode” or power supply only The size can be several orders of magnitude smaller than when directly energized.

Typical values are as follows:
Magnet inductance = 100 Henry magnet resistance = 10 ⁻⁷ Ω
Resistor 5 = 10 ^-6 Ω
I power supply = 100 amperes ΔI overcurrent = 10 amperes A magnet that normally operates in “permanent mode” exhibits a time constant of 10 ⁻⁹ seconds or a decay rate of 3.6 ppm / hour.

The same magnet operating in “quasi-permanent” mode using resistor 5 as described above has a magnetic field stability of 3.6 × 10 ⁻⁴ ppm / hour for a power supply variation of 10 ⁻⁵ , 10 ^−4. The magnetic field stability of 3.6 × 10 ⁻³ ppm / hour is exhibited with respect to fluctuations in power supply. Therefore, it is the instability of the power supply current that dominates the magnetic field stability of this latter mode. By the way, it is understood that when the power source remains connected in the permanent mode, the time constant of the circuit is small, so that a much larger magnetic field instability occurs than in the quasi-permanent mode.

  In order for the desired attenuation to reach zero, the current change ΔI needs to be set correctly. There are various ways in which this can be achieved.

  In the first approach, an additional superconducting switch 6 can be connected in parallel with the switch 3 and the resistor 5. Initially, when the power supply 4 is activated, the magnet 1 is powered up to the desired field strength, the switch 6 is closed, and the power supply is deactivated. The magnetic field attenuation is then monitored, for example using conventional NMR techniques (step 13), from which the magnet attenuation can be calculated by measuring the change in NMR resonance frequency over time, which is then the change in magnetic field over time. Used to determine rate. Once the magnet inductance and magnet operating current are known, the equivalent magnet resistance voltage can be calculated. The magnet resistance voltage is then divided by the value of resistor 5 and the value of increased current ΔI is obtained from the power supply using equation [1] above. Then, the switch 6 is opened, and after the switch 3 is closed, the above-described process is performed by applying a pre-calculated additional current ΔI.

  In the second method, a voltmeter (not shown) can be attached to both ends of the magnet 1 in order to determine the resistance 2 of the magnet 1.

  In the third approach, a rough value of ΔI is provided (step 12) and magnetic field attenuation or drift is measured in step 13. If the drift is too great (step 14), the power supply is increased and the processes of steps 12 and 13 are repeated. This set of steps can be repeated until the required field attenuation is achieved.

  Needless to say, in this case, it is assumed that an increase in current is required to achieve the required field attenuation or drift, but since a reduction in current may be necessary, step 12 is Adjusted accordingly.

  Next, the quasi-permanent mode will be described in more detail.

Usually, in the known method, the magnet damping prevails by the magnet resistor 2 (R ₁ ) in series with the magnet in the permanent mode. In this situation, the voltage drop due to the change in the current of the magnet inductor is equivalent to the voltage drop of the magnet resistor 2. Ie

Here, L is the magnet inductance, I ₁ is the current flowing through the magnet, and R ₁ is the magnet resistance 2.

  Thus, for a particular magnet, the NMR proton frequency is proportional to the magnet current, so the attenuation Δf of the operating proton frequency f of the magnet is given by:

For example, for a magnet with frequency f = 400 MHz, L = 58 Henry, and nominal R ₁ = 4 μΩ, this results in a theoretical frequency attenuation factor of approximately 100,000 PHz / hour (“PHz / hour” is the attenuation of the proton resonant frequency) Represents).

In contrast to the above, in the quasi-permanent mode, the current source 4 remains connected to the magnet and the switch 3 is closed so that current flows through the magnet 1 and at the same time the switch 3 and the resistor 5. Because the power supply remains connected, it magnet resistance 2 in addition to the DC current I ⁰ ₁ flowing to the (here has a resistance value expressed as R _1), the DC current I ⁰ ₂ a resistor 5 ( Having a resistance R ₂ ). During the static mode, the voltage generated on R ₂ should be the same as in the case of magnet resistance R ₁ . Therefore, the voltages are equal, so that

The change δI ₂ in the current I ₂ (t) = (I ⁰ ₂ + δI ₂ ) of the switch 3 and the resistor 5 is accompanied by the time change δI ₁ of the current I ₁ (t) = (I ⁰ ₁ + δI ₁ ). Or balanced by it. The power source is maintained in an operating state, and therefore, the decisive factor in determining the decay rate is the stability of the power source. To take this further into account, a small mathematical notation is adopted here.

  As a result of the small change in current resulting from slight instability of the power supply 4, the voltage balance calculation yields

  Due to the reduction of the terms:

Further, since the total current I is I ₁ + I ₂ , the total change in current is as follows.

Substituting δI ₂ = δI−δI ₁ gives the following.

  Rearrange the terms as follows:

The stability of the current source is most important. For a power supply with a current stability of 10 ppm / hour, the change δI ₁ is reduced to 3.6 × 10 ⁻⁴ ppm / hour. In the case of time δ _t << L / (R ₁ + R ₂ ), δI ₁ is obtained by the following equation.

To test the above analysis, an experimental superconducting magnet with a resistance close to zero and an inductance of 57.52 Henry was deliberately placed in series with a 4 μΩ finite nominal resistance R ₁ . The decay rate was measured under operating conditions in both permanent and quasi-permanent modes.

  In permanent mode, the magnet was operated with a current of 95.5 A at a proton frequency of 400.419 MHz, resulting in a voltage drop of 0.382 mV across the 4 μΩ resistor. The resulting decay rate was measured as 111,000 PHz / hour.

  In quasi-permanent mode, a 90 μΩ resistor (resistor 5 in FIG. 1) was placed in parallel with the magnet (and thus in series with switch 3). To account for parallel resistance 2, an increased current of 99.256 A was used. This results in a measured attenuation factor of +49 PHz / hour, indicating that the current has become slightly larger than the optimum value, so that the proton frequency actually increases. However, it can be seen that the overall rate of change of the proton frequency is substantially reduced. Thus, an improved value can be achieved by using a slightly smaller current of 99.254A. This result demonstrates that even with a magnet resistance as high as 4 μΩ, an attenuation factor of 0.01 ppm / hour (as described above) can be achieved with the present invention.

  Using the above equation to generate a voltage of 0.382 mV across a 90 μΩ resistor requires a current of 4.24 A resulting in a total current of 99.7 A.

  Assuming a power supply current drift of 10 ppm / hour for a current of 99.7 A (ie current suitable for 400 MHz operation), the expected instability rate of the current source is about 1 mA / hour.

Using δI / δt = ImA / hour with R ₂ = 90 μΩ, the rate of change of the magnet current is δI / δt = 5.6 × 10 ⁻⁶ A / hour.

  This is equal to the calculated attenuation rate of 23 PHz / hour.

Therefore, it can be seen that the magnetic field stability can be considerably improved by providing the parallel resistance R ₂ and using the power source during operation of the magnet.

  As a further test using an experimental magnet system, the current was reduced by 2 mA to simulate a change in power supply current. No step evidence corresponding to this change is found in the attenuation trace, only a small change in the attenuation slope of 34 PHz / hour, which is consistent with the large time constant of the magnet circuit.

In some superconducting magnets, the resistance (R ₁ ) of the magnet itself is very small, for example 10 ⁻¹⁰ Ω to 10 ⁻¹³ Ω, so that a very long time constant is generated in the magnet circuit in the permanent mode. However, other superconducting magnets have higher resistance values. One particular example of these is high temperature superconductors with “finite” resistance, so such magnets are more likely to cause greater instability in their magnetic fields. The fabrication process can also cause an increase in resistance of more traditional low temperature superconducting materials. For these types of magnets having finite resistance values, the present invention is particularly suitable because the time constant of the magnet circuit can be significantly reduced.

  The prior art published in US 2003/0057942 has been described above, but the present invention will now be described.

  The solution described in US 2003/0057942 is subject to at least the following potential drawbacks. The present invention seeks to provide an improved superconducting magnet current stabilization circuit to alleviate one or more of these disadvantages.

  The solution described in US 2003/0057942 is suitable for application to magnets having separate protection circuits for the various sections of the magnet, but protected by a single protection circuit. Not applicable to magnets. The above-described arrangement for mitigating magnet drift is only effective when the voltage at switch 3 and stability resistor 5 is less than a few tens of volts, otherwise excessive heating and current will cause switch 3 to Destroy. Such a configuration is prone to damage when a quench occurs, as will now be described.

  Consider the case of a superconducting magnet 1 that is energized up to 1000 A and has, for example, a 2Ω parallel protective resistor connected across the associated switch 3. During the quench, a current of about 1000 A begins to flow through the 2Ω resistor, which generates a voltage of about 2 kV on magnet 1 and switch 3. Obviously, the voltage and thus the heating power is so great that it is impossible to use such switches and protective resistors for such magnets. The resistance of the superconducting switch 3 in the resistance mode can be between several ohms and several hundred ohms.

  As such, conventional superconducting fault current limiters (SFCL) are used in the distribution industry to prevent damage to the distribution network due to excessive current flow, for example due to short circuits. Several different types of SFCL are known, such as resistive, inductive, and rectifier types. Such types of comparisons were published in Journal of Physics: Conference series 43 (2006) 909-912 (A. Morandi et al.). As is known, superconductors have zero electrical resistance when operating within certain limits of temperature, magnetic field, and current density. When these quantities, which differ for each superconducting material, exceed a certain value, the superconductor returns to a “normal” resistance state. Various types of SFCL take advantage of this feature to provide a current limiting device that can handle hundreds of amps of current at kilovolt potentials. Some types of SFCL respond to excessive current, magnetic field, or temperature by limiting the current through the device to the current level. Other types react by reducing the current to a relatively low level or zero.

1 is a schematic block diagram of an apparatus described in U.S. Patent Application Publication No. 2003/0057942. 3 is a flow diagram illustrating an example of a method described in US Patent Application Publication No. 2003/0057942. 1 shows a schematic block diagram of an apparatus according to an embodiment of the present invention. FIG. 3 shows a schematic block diagram of an apparatus according to another embodiment of the present invention. FIG. 3 shows a schematic block diagram of an apparatus according to another embodiment of the present invention.

  The above and further objects, features and advantages of the present invention will become more apparent from the following description of specific embodiments, given by way of example only, in conjunction with the accompanying drawings.

  The described prior art solution can be applied to configurations made up of a large number of circuits, each with a small magnet or each protected by a protective resistor. If the entire magnet is protected by only one resistor, usually outside the cryostat but can also be provided inside the cryostat, the prior art solution is no longer sufficient for at least the following reasons. During natural quenching of a superconducting magnet, several kilovolts are generated between the beginning and end of the magnet coil. Conventional superconducting switches such as those used in superconducting magnets (eg, MRI magnets) are not made to withstand such extreme conditions.

  The present invention addresses this problem by providing a stabilization circuit applicable in such situations. In particular, the stabilization circuit of the present invention uses a superconducting fault current limiter that interrupts current above a certain level. This can be done by limiting the current to a certain maximum value or by reducing the current to a lower value, which may be zero.

  The present invention, in a sense, is similar to the configuration of US 2003/0057942, but is applicable to superconducting magnets that are less susceptible to damage during a quench event and that have a single protection circuit. Provided is a current stability circuit for a superconducting magnet.

  A circuit according to an embodiment of the present invention is shown in FIG. The present invention provides a superconducting magnet current drift by providing a superconducting fault current limiter 7 in series with a stabilizing resistor 5 and in parallel with a protected magnet 1 itself having a magnet coil and a resistor 2. A stabilization circuit for reducing or eliminating is proposed. A connecting means 9 is provided, whereby the magnet 1 connected in parallel with the series combination of the superconducting fault current limiter 7 and the stabilizing resistor 5 can be further connected in parallel with the DC power source 4.

  Basically, the superconducting fault current limiter 7 replaces the switch 3 of the prior art US 2003/0057942 (FIG. 1). However, when a quench occurs, the superconducting fault current limiter 7 is strong enough to withstand the high currents and voltages it receives, and in extreme load situations its characteristics change to The flowing current is shunted to the protective resistor 8, where the energy stored in the magnet is dissipated. A superconducting fault current limiter is a device that can withstand applied voltages and currents far exceeding the limits of a superconducting switch. For example, known superconducting current fault current limiters can withstand thousands of amps and kilovolts without damage.

  Once the current reaches a sufficiently high value and the included superconductor becomes resistive due to excessive current density, excessive magnetic field, or excessive temperature, the superconducting current fault current limiter will reduce the current flowing through them. Work to limit. The circuit of FIG. 3 shows a protection circuit in the form of a protection resistor 8 which can be arranged outside the cryostat, for example. This can be achieved by a single resistor or an array of multiple resistors. These are preferably arranged outside the cryostat in order to minimize the evaporation loss of cryogen or to keep the temperature of the cryogen-free cryostat at a minimum. The protective resistor 8 provides a single protective configuration for the entire magnet 1.

  Both the prior art switch 3 and the superconducting fault current limiter 7 of the present invention are superconducting devices. They each work on the principle that their resistance is zero in the superconducting state and then when they exceed a critical current or temperature they exhibit a high resistance. The basic difference between the two devices is that the superconducting fault current limiter is more resistant to high currents and voltages and is therefore more robust.

  Superconducting fault current limiters are components known per se and are commonly used to detect and isolate faults in distribution circuits. It works as follows. The superconducting wire is cooled to a temperature at which superconducting is possible. During normal operating conditions, current below the critical current density flows through the superconducting wire and associated circuitry. The critical current density is a current density value that, when flowing through the superconducting wire, stops the superconducting and returns to the normal resistance mode regardless of the temperature. During a fault (a quench event in the present invention) condition, overcurrent is passed through the superconducting wire of the superconducting fault current limiter. The superconducting fault current limiter is configured such that this overcurrent exceeds the critical current density. Overcurrent causes the superconducting wire to stop superconducting and become resistive. The superconducting wire and any conductive cladding applied to the superconducting wire are configured so that their impedance is sufficiently high to limit the current flowing therethrough to a level that is safe for the associated circuitry. A parallel resistive conductive path can be provided to pass a portion of the current in this state. In the present invention, such a parallel resistive path is provided at least by the protective resistor 8. In general, a superconducting fault current limiter maintains its high impedance state while current flows through it, as its impedance ensures that it is maintained above its critical temperature. When current flow stops, typically because the circuit is turned off after service engineer intervention or because of reset circuit operation, the superconducting fault current limiter is cooled down to a temperature where superconducting is possible, and the superconducting The fault current limiter will again be able to operate at any time in its normal state.

  Such operation typically causes excessive current to flow in a fault condition in a power distribution system, as described, for example, in Canadian Patent No. 2070322 and Journal of Physics: Conference series 43 (2006) 909-912 (A. Morandi et al.). Used to avoid.

  The present invention uses such a superconducting fault current limiter to maintain the stability of the magnetic field strength in a new application, namely a superconducting magnet.

The superconducting fault current limiter (SFCL) envisioned by the present invention can be made from any type of superconducting material, HTS, MgB ₂ , or LTS. HTS is preferred because it allows the SFCL to be placed in a high temperature region that does not dissipate too much cryogen and cut off at low currents. The SFCL can be cooled independently by a cryocooler so that it shuts off fairly quickly.

  FIG. 3 schematically illustrates an embodiment of the present invention. In a preferred embodiment of the present invention, the high power protection resistor 8 is placed outside the cryostat holding the superconducting magnet and is connected to the magnet in the cryostat and the superconducting fault current limiter with a cable. Is preferred. It is also possible to place the external resistor in a separate compartment or inside the magnet cryostat. The protective resistor is preferably cooled, for example with air or water cooling or other refrigerant, in order to effectively dissipate energy from the magnet.

  In the context of a typical DC actuated superconducting magnet, a series superconducting fault current limiter 7 used in place of the switch in the prior art resistor stabilization solution limits the current during quenching and protects it. Divert to 8.

  Connection means 9 are provided to allow connection and disconnection of the parallel DC power supply to the magnet and to the series combination of superconducting fault current limiter 7 and resistor 5. Such connecting means can include, for example, plugs, sockets, terminal boards, exposed conductors, permanent (superconducting) joints, and the like. The DC power source 4 is connected to the connection means when the magnet is used.

  Thus, the present invention uses a superconducting fault current limiter to achieve permanent stability and quench protection of the superconducting magnet.

  FIG. 4 shows an alternative embodiment of the present invention. In this second embodiment, a further superconducting fault current limiter 7 a is arranged in series between the connection means 9 and the magnet 1. Even when such a superconducting fault current limiter 7a is used in series with the power source 4, the quenching of the magnet essentially opens the further superconducting fault current limiter 7a so that the power source 4 is isolated and the protective resistor Since only 8 continues to connect to the magnet, it protects the power supply 4 and helps to allow the magnet to be energized by a standard 10V power supply.

  As shown, in this embodiment, a further superconducting fault current limiter 7 a is arranged in series between the connection means 9 and the magnet 1. The further superconducting fault current limiter 7a is preferably arranged in series between the magnet 1 and the series combination of the fault current limiter 7 and the resistor 5. The magnet 1, the further superconducting fault current limiter 7a, the fault current limiter 7 and the resistor 5 form a series closed circuit.

  FIG. 5 shows a third embodiment of the present invention with a certain similarity to the embodiment of FIG. In this third embodiment, the further superconducting fault current limiter 7a of FIG. 4 connects the connecting means 9 and the magnet 1, the protective resistor 8, and the series combination of the fault current limiter 7 and the resistor 5. Move to a new position in series with the node. Similar to the embodiment of FIG. 4, when such an additional superconducting fault current limiter 7a is used in series with the power supply 4, the magnet quench essentially opens the superconducting fault current limiter 7, 7a. Thus, the power supply 4 is isolated and only the protective resistor 8 continues to connect to the magnet, thus protecting the power supply 4 and helping to energize the magnet with a standard 10V power supply.

  As shown, in this embodiment, the power supply 4, the series combination of fault current limiter 7 and resistor 5, and the further superconducting fault current limiter 7a form a series closed circuit.

Claims (5)

A superconducting magnet (1) for generating an operating amount of magnetic field under operating conditions; and a connecting means (9) for connecting the magnet in parallel with a DC power source (4) , whereby the operating magnet In a superconducting magnet assembly configured such that a magnet is energized by the power source to generate an operational amount of a desired magnetic field ;
The superconducting magnet is connected in parallel with a series combination of a superconducting fault current limiter (7) and a resistor (5) and further in parallel with a protective resistor (8), so that under quench conditions, and wherein the superconducting fault current limiter (7) is a current I by the Rukoto such as resistance to flow the protective resistor (8), made so as to dissipate energy from the superconducting magnet superconducting magnet assembly.   The DC power supply (4) is connected to the connection means in parallel with the magnet and in parallel with a series combination of the fault current limiter (7) and the resistor (5). Superconducting magnet assembly. Superconducting magnet assembly according to claim 1 or 2 , wherein the resistor (5) has a resistance in the range of 1-1000 times the resistance (2) of the magnet (1). It said resistor (5) has a resistance of 10 to 100 fold range of resistance (2) of the magnet (1), the superconducting magnet assembly according to any one of claims 1 to 3. The power supply, the magnet, and the resistor is configured to instability of the magnetic field generated during use is substantially 10ppm / less time, the superconducting magnet assembly according to any one of claims 1 to 4 .

Images